183_notes:energy_dissipation

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183_notes:energy_dissipation [2014/10/31 13:19] – [Where does the energy go?] caballero183_notes:energy_dissipation [2021/06/02 23:15] (current) – [Air Resistance] stumptyl
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-===== Dissipation of Energy =====+Section 7.10 in Matter and Interactions (4th edition) 
  
-You have read that [[183_notes:energy_cons|energy is always conserved]]. This is a true observable fact of the universe. Energy cannot be created or destroyed, it simply changes forms. However, sometimes those forms are less useful to us. For example, the increased thermal energy of a box due to the frictional interaction with the surface it is pushed across is unlikely to be useful. This type of transformation of energy is often referred to as "dissipating" energy. In these notes, you will read about one form of energy dissipation that is due to collisions with air molecules: air resistance.+===== Dissipation of Energy =====
  
 +You have read that [[183_notes:energy_cons|energy is always conserved]]. This is a true observable fact of the universe. Energy cannot be created or destroyed, it simply changes forms. However, sometimes those forms are less useful to us. For example, the increased thermal energy of a box due to the frictional interaction with the surface it is pushed across is unlikely to be useful. This type of transformation of energy is often referred to as "dissipating" energy. **In these notes, you will read about one form of energy dissipation that is due to collisions with air molecules: air resistance.
 +**
 ==== Air Resistance ==== ==== Air Resistance ====
  
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 Let's say you dropped a metal ball from rest. Below is a set of frames (taken at equal time intervals) from a video of a metal ball being dropped straight down. Notice the ball's displacement increases as each time step elapses. The effect of air resistance is very small. To a reasonable degree, we can [[183_notes:constantf|model this motion using constant force]]. Let's say you dropped a metal ball from rest. Below is a set of frames (taken at equal time intervals) from a video of a metal ball being dropped straight down. Notice the ball's displacement increases as each time step elapses. The effect of air resistance is very small. To a reasonable degree, we can [[183_notes:constantf|model this motion using constant force]].
  
-{{ 183_notes:mi3e_07-039.jpg?400 }}+{{ 183_notes:week10_dissipation1.png?400 }}
  
 If you instead dropped a coffee filter, you would observe something all together different. The frames below are taken from a video of a coffee filter dropped from rest. Notice that the displacement between each frame is roughly the same (especially near the end of the video). This latter motion could be modeled to a reasonable degree [[183_notes:displacement_and_velocity|using constant velocity motion]]. If you instead dropped a coffee filter, you would observe something all together different. The frames below are taken from a video of a coffee filter dropped from rest. Notice that the displacement between each frame is roughly the same (especially near the end of the video). This latter motion could be modeled to a reasonable degree [[183_notes:displacement_and_velocity|using constant velocity motion]].
  
-{{ 183_notes:mi3e_07-040.jpg?600 }}+{{ 183_notes:week10_dissipation2.png?600 }}
  
 ==== Where does the energy go? ==== ==== Where does the energy go? ====
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 $$\underbrace{\Delta K_{filter}}_{0\mathrm{\:in\:later\:frames}} + \Delta U _{grav} = W_{surr}$$ $$\underbrace{\Delta K_{filter}}_{0\mathrm{\:in\:later\:frames}} + \Delta U _{grav} = W_{surr}$$
  
-$$W_{surr} = \Delta U _{grav} $$+The kinetic energy of the coffee filter doesn't change much after a short while because the forces acting on the filter are balanced. That is, the force gravitational force and the force of the air are the same size. This results in a condition called [[http://en.wikipedia.org/wiki/Terminal_velocity|terminal velocity]], which is also a [[http://www.imdb.com/title/tt0111400/|terrible film]].
  
-What can do work on the coffee filter if the Earth is in the system? The air molecules that collide with the coffee filter as it falls down. These molecules are struck by the filter on the way down and have their kinetic energy increased. The energy of the Earth-filter system is dissipated by the air. The air molecules gain kinetic energy, which cannot really be used for anything useful.+$$\vec{F}_{net} = \vec{F}_{grav} + \vec{F}_{air} = 0$$ 
 +$$\vec{F}_{grav} = -\vec{F}_{air} \rightarrow F_{grav} = F_{air} $$ 
 +$$ mg = cv_{terminal}^2 \rightarrow v_{terminal} = \sqrt{\dfrac{mg}{c}}$$ 
 + 
 +where $c$ is a constant that contains all the constants in the [[183_notes:drag|turbulent drag force formula]]. As a result, the work done by the surroundings is equal to the change in gravitational potential energy. 
 + 
 +$$W_{surr} = \Delta U _{grav} $$
  
 +//__What can do work on the coffee filter if the Earth is in the system? The air molecules collide with the coffee filter as it falls down. These molecules are struck by the filter on the way down and have their kinetic energy increased.__// The energy of the Earth-filter system is dissipated by the air. The air molecules gain kinetic energy, which cannot really be used for anything useful.
  
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